Publication:
Spectral singularities in the TE and TM modes of a PT-symmetric slab system: optimal conditions for realizing a CPA-laser

dc.contributor.coauthorN/A
dc.contributor.departmentDepartment of Mathematics
dc.contributor.departmentDepartment of Mathematics
dc.contributor.kuauthorMostafazadeh, Ali
dc.contributor.kuauthorSarısaman, Mustafa
dc.contributor.kuprofileFaculty Member
dc.contributor.kuprofileResearcher
dc.contributor.otherDepartment of Mathematics
dc.contributor.schoolcollegeinstituteCollege of Sciences
dc.contributor.schoolcollegeinstituteCollege of Sciences
dc.contributor.yokid4231
dc.contributor.yokid217652
dc.date.accessioned2024-11-09T22:59:33Z
dc.date.issued2016
dc.description.abstractAmong the interesting outcomes of the study of the physical applications of spectral singularities in PT-symmetric optical systems is the discovery of CPA-lasers. These are devices that act both as a threshold laser and a coherent perfect absorber (CPA) for the same values of their physical parameters. Unlike a homogeneous slab that is made to act as a CPA, a slab CPA laser would absorb the incident waves coming from the left and right of the device provided that they have appropriate intensity and phase contrasts. We provide a comprehensive study of one of the simplest experimentally accessible examples of a CPA laser, namely a PT-symmetric optical slab system consisting of a balanced pair of adjacent or separated gain and loss components. In particular, we give a closed form expression describing the spectral singularities of the system which correspond to its CPA laser configurations. We determine the intensity and phase contrasts for the TE and TM waves that are emitted (absorbed) whenever the slab acts as a laser (CPA). We also investigate the behavior of the time-averaged energy density and Poynting vector for these waves. This is necessary for determining the optimal values of the physical parameters of the system that make it act as a CPA laser. These turn out to correspond to situations where the separation distance s between the gain and loss layers is an odd multiple of a characteristic length scale so. A curious by-product of our study is that, except for the cases where s is an even integer multiple of so, there is a critical angle of polarization beyond which the energy of the waves emitted from the lossy layer can be larger than the energy of those emitted from the gain layer.
dc.description.indexedbyWoS
dc.description.indexedbyScopus
dc.description.openaccessYES
dc.description.publisherscopeInternational
dc.description.sponsoredbyTubitakEuTÜBİTAK
dc.description.sponsorshipScientific and Technological Research Council of Turkey (TUBITAK) [112T951]
dc.description.sponsorshipTurkish Academy of Sciences (TUBA) We are grateful to Aref Mostafazadeh, Alphan Sennaroglu, and Ali Serpenguzel for fruitful discussions. This work has been supported by the Scientific and Technological Research Council of Turkey (TUBITAK) in the framework of the project no: 112T951, and by the Turkish Academy of Sciences (TUBA).
dc.description.volume375
dc.identifier.doi10.1016/j.aop.2016.09.008
dc.identifier.eissn1096-035X
dc.identifier.issn0003-4916
dc.identifier.quartileQ2
dc.identifier.scopus2-s2.0-84992197923
dc.identifier.urihttp://dx.doi.org/10.1016/j.aop.2016.09.008
dc.identifier.urihttps://hdl.handle.net/20.500.14288/7912
dc.identifier.wos389788100016
dc.keywordsSpectral singularity
dc.keywordsPT-symmetry
dc.keywordsLaser threshold condition
dc.keywordsCoherent perfect absorption
dc.keywordsCPA-laser
dc.languageEnglish
dc.publisherAcademic Press Inc Elsevier Science
dc.sourceAnnals of Physics
dc.subjectPhysics
dc.titleSpectral singularities in the TE and TM modes of a PT-symmetric slab system: optimal conditions for realizing a CPA-laser
dc.typeJournal Article
dspace.entity.typePublication
local.contributor.authorid0000-0002-0739-4060
local.contributor.authorid0000-0002-7148-0836
local.contributor.kuauthorMostafazadeh, Ali
local.contributor.kuauthorSarısaman, Mustafa
relation.isOrgUnitOfPublication2159b841-6c2d-4f54-b1d4-b6ba86edfdbe
relation.isOrgUnitOfPublication.latestForDiscovery2159b841-6c2d-4f54-b1d4-b6ba86edfdbe

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